In this experiment, you will investigate total internal reflection using a semicircular glass block. You directs a narrow ray of light from a ray box into t...

Assessment: Physics (9-1) 0972 | Paper 5 Mock 01 | Practical Test Subject: Physics (9-1) - 0972

Question 1 Report

In this experiment, you will investigate total internal reflection using a semicircular glass block. You directs a narrow ray of light from a ray box into the curved surface of the block so that the ray passes through the glass and arrives at the centre of the flat surface, point O. The apparatus is shown in Fig. 5.1.

You gradually increases the angle of incidence at the flat surface by rotating the ray box. At a certain angle, the refracted ray disappears and the light is totally internally reflected. You records this angle as the critical angle c. The ray-trace diagram for the critical angle is shown in Fig. 5.2.

diagram

(a) Using Fig. 5.2, measure and record the critical angle c. [1]

(b) Calculate sin c. [1]

(c) Calculate the refractive index n of the glass using the equation n = 1 / sin c. [2]

(d) State why the ray of light must enter through the curved surface of the block, directed towards the centre of the flat surface. [1]

(e) Describe what happens to the ray at the flat surface when the angle of incidence is less than the critical angle. [2]

(f) Describe what happens to the brightness of the refracted ray as the angle of incidence is increased towards the critical angle. [1]

(g) State one practical use of total internal reflection. [1]

(h) The critical angle for diamond is 24°. Calculate the refractive index of diamond. [1]

Answer Details

(a) From Fig. 5.2, the critical angle c is measured between the incident ray and the normal at the flat surface at point O. Using a protractor on the diagram:

\[ c = 42^\circ \] [1]

(Accept 41° to 43°.)

(b) Calculating the sine of the critical angle:

\[ \sin c = \sin 42^\circ = 0.669 \] [1]

(Accept a value consistent with the measured angle.)

(c) The refractive index of the glass is found using \( n = 1 / \sin c \):

\[ n = \frac{1}{\sin c} \] [1]

\[ n = \frac{1}{0.669} = 1.49 \] [1]

(Accept 1.4 to 1.6 if consistent with the measured critical angle.) This value is typical for glass, confirming the measurement is reasonable.

(d) The ray must enter through the curved surface because at the curved surface, the ray travels along a radius of the semicircle, which means it hits the curved surface at right angles (perpendicular to the surface). A ray striking a surface perpendicularly does not refract, so it passes straight through to the flat surface without changing direction. [1]

This ensures that refraction occurs only at the flat surface, so the measured angle of incidence at the flat surface is the true angle.

(e) When the angle of incidence at the flat surface is less than the critical angle:

  • The ray is partly refracted as it passes from the glass into the air. The refracted ray bends away from the normal (since glass is optically denser than air). [1]
  • At the same time, a weak reflected ray is also produced inside the glass block. This partial reflection always accompanies refraction. [1]

(f) As the angle of incidence increases towards the critical angle, the refracted ray becomes dimmer (less bright). [1]

More and more of the light energy is reflected rather than refracted. At the critical angle, the refracted ray just grazes along the surface (at 90° to the normal), and beyond this angle, all the light is reflected.

(g) One practical use of total internal reflection (any one): [1]

  • Optical fibres for telecommunications or medical endoscopes: light is guided along the fibre by repeated total internal reflection.
  • Reflecting prisms in binoculars, periscopes, or SLR cameras.
  • Bicycle reflectors and road reflectors.

(h) For diamond, the critical angle is 24°:

\[ n = \frac{1}{\sin 24^\circ} = \frac{1}{0.407} = 2.46 \] [1]

Diamond has a much higher refractive index than glass (2.46 compared to about 1.5), which means it has a much smaller critical angle. This causes extensive internal reflection, producing the characteristic sparkle of a cut diamond.

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